MR tomography method and apparatus for performing the method

Claim 2

An Mr tomography method wherein echo signals are extracted during a plurality of sequences for the reconstruction of the spatial density distribution in an examination region, each execution of a sequence including a selection phase during which a single high-frequency pulse is applied to the examination region in the presence of a magnetic gradient field, a subsequent encoding phase during which the examination region is exposed to a magnetic gradient field with a gradient which varies as regards magnitude or direction from one sequence to another, and a subsequent read phase during which the spin echo signal generated in the examination region is sampled in the presence of a magnetic gradient field, after which an image which is dependent on the proton distribution is calculated from the echo signal, the image values for the individual pixels of the image being determined by formation of the absolute value during a final step, characterized in that each sequence is executed twice, the gradient field (Gx) during the read phase in the second execution of each sequence, or the gradient field previously extending in the opposite direction, being proportioned so that the distance in time between the high-frequency pulse and the echo signal in the second execution is shifted with respect to the first sequence over a period of time (T) which corresponds to half the reciprocal value of the difference between the Larmor frequencies (df) of water-bound and fat-bound hydrogen protons, respectively, an image of the density distribution in the examination region being calculated from the sums of or the differences between the echo signals formed during the two executions of the sequences.

Claim 3

An MR tomography method wherein echo signals are extracted during a plurality of sequences for the reconstruction of the spatial density distribution in an examination region, each execution of a sequence including a selection phase during which a single high-frequency pulse is applied to the examination region in the presence of a magnetic gradient field, a subsequent encoding phase during which the examination region is exposed to a magnetic gradient field with a gradient which varies as regards magnitude or direction from one sequence to another, and a subsequent read phase during which the spin echo signal generated in the examination region is sampled in the presence of a magnetic gradient field, after which an image which is dependent on the proton distribution is calculated from the echo signal, the image values for the individual pixels of the image being determined by formation of the absolute value during a final step, characterized in that each sequence includes two read phases (t2-t3', t4'-t5') during which the gradient field has the same direction, each of the read phases being preceded by a period of time during which the gradient field extends in the opposite direction with respect to its direction during the read phase, the variation in time of the gradient field (Gx) being chosen so that the echo signal occurring during the second read phase is shifted with respect to the echo signal occurring the first read phase over a period of time (T') which corresponds to half the reciprocal value of the difference between the Larmor frequencies (df) of water-bound and fat-bound hydrogen protons, respectively, or to an odd multiple thereof, an image of the density distribution in the examination region being calculated from the sums of or the differences between the echo signals formed during the two read phases.

Claim 4

An MR tomography method wherein echo signals are extracted during a plurality of sequences for the reconstruction of the spatial density distribution in an examination region, each execution of a sequence including a selection phase during which a single high-frequency pulse is applied to the examination region in the presence of a magnetic gradient field, a subsequent encoding phase during which the examination region is exposed to a magnetic gradient field with a gradient which varies as regards magnitude or direction from one sequence to another, and a subsequent read phase during which the spin echo signal generated in the examination region is sampled in the presence of a magnetic gradient field, after which an image which is dependent on the proton distribution is calculated from the echo signal, the image values for the individual pixels of the image being determined by formation of the absolute value during a final step, characterized in that each sequence includes two read phases (t2-t3', t4'-t5') during which the gradient field has the same direction, each of the read phases being preceded by a period of time during which the gradient field extends in the opposite direction with respect to its direction during the read phase, the variation in time of the gradient field (Gx) being chosen so that the echo signal occurring during the second read phase is shifted with respect to the echo signal occurring the first read phase over a period of time (T') which corresponds to half the reciprocal value of the difference between the Larmor frequencies (df) of water-bound and fat-bound hydrogen protons, respectively, or to an odd multiple thereof, an image of the density distribution in the examination region being calculated from the sums of or the differences between the echo signals formed during the two read phases.

Claim 5

A method as claimed in claim 1, characterized in that the gradient field has the same magnitude during the read phase of both executions of a sequence, the distance in time between the gradient field and the high-frequency pulse in one sequence exceeding that in the other sequence by a period of time (T) which amounts to half the reciprocal value of the difference between the Larmor frequencies of water-bound and fat-bound hydrogen protons, respectively.

Claim 6

A method as claimed in claim 1, characterized in that during the read phase the gradient field in one sequence is lrger than that in the other sequence.

Claim 8

An appartatus for performing the method claimed in claim 1, including means (1) for generating steady, uniform magnetic field, a high-frequency coil system (11) for generating high-frequency pulses, gradient coils (3, 5, 7) for generating magnetic fields which extend in the direction of the steady field and which have gradients in the same direction as well as in the direction perpendicular thereto, a sampling device (28 . . . 31) for receiving echo signals generated in an examination region, a control unit (45) for controlling the gradient coils, the high-frequency ccoil system and the sampling device, as well as a reconstruction unit (35) which calculates an image of the spatial spin distribution from the echo signals, characterized in that the control unit (45) is programmed so that each sequence is executed twice, the gradient coils (3, 5, 7) being controlled so that the distance between the echo signals and the high-frequency pulse is shifted over a period of time (T) which corresponds to half the reciprocal value of the difference between the fat frequency and the water frequency, the reconstruction unit (35) being constructed so that it determines the image on the basis of the sum or the difference between the echo signals.

Claim 9

An apparatus for performing the method claimed in claim 2, including means (1) for generating a steady, uniform magnetic field, a high-frequency coil system (11) for generating high-frequency pulses, gradient coils (3, 5, 7) for generating magnetic fields which extend in the direction of the steady field and which have gradients in the same direction as well as in the direction perpendicular thereto, a sampling device (28 . . . 31) for receiving echo signals generated in an examination region, a control unit (45) for controlling gradient coils, the high-frequency coil system and sampling device, as well as a reconstruction unit (35) which calculates an image of the spatial spin distribution from the echo signals, characterized in that the control unit is programmed so that each sequence includes two read phases (t2-t3'; t4'-t4'-t5') during which the gradient field has the same direction, each of the read phases being preceded by a period of time during which the gradient field extends in the opposite direction with respect to its direction during the read phase, the variation in time of the gradient field (Gx) being chosen so that the echo signal occurring during the second read phase is shifted with respect to the echo signal occurring during the first read phase over a period of time (T') which corresponds to half the reciprocal value of the difference between the Larmor frequencies (df) of water-bound and fat-bound hydrogen protons, respectively, or to an odd multiple thereof, the reconstruction unit (35) being constructed so that it determines the image on the basis of the sum of or the difference between the echo signals.